Abstract

By using the finite-temperature quantum field theory, we calculate the finite-temperature effective potential and extend the improved quark mass density-dependent model to finite temperature. It is shown that this model can not only describe the saturation properties of the nuclear matter, but also explain the quark deconfinement phase transition successfully. The critical temperature is given and the effect of the ω-meson is addressed.

Highlights

  • Quark- meson coupling(QMC) model suggested by Guichon [1] is a famous hybrid quark meson model, which can describe the saturation properties of nuclear matter and many other properties of nuclei successfully

  • The nuclear system was suggested as a collection of MIT bag, ω- meson and σ- meson and the interactions between quarks and mesons are limited within the MIT bag regions because the quark cannot escape from the MIT bag

  • The reason is that the interactions between quarks and mesons are limited within the bag regions, the multireflection of quarks and mesons by MIT bag boundary must be taken into account for getting the free propagators

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Summary

INTRODUCTION

Quark- meson coupling(QMC) model suggested by Guichon [1] is a famous hybrid quark meson model, which can describe the saturation properties of nuclear matter and many other properties of nuclei successfully. The QMC model is successful in describing many physical properties of nuclear systems, but as was pointed in our previous paper [6], it has two major shortcomings: (1) It is a permanent quark confinement model because the MIT bag boundary condition cannot be destroyed by temperature and density. It cannot describe the quark deconfinement phase transition. These two shortcomings inherited from the MIT bag To overcome these two shortcomings, in our previous paper [6], we suggested an improved quark mass density- dependent(QMDD) model. Since instead of the MIT bag in QMC model, a FL soliton bag is introduced in IQMDD model, we can use our model to discuss the quark deconfinement phase transition.

THE IQMDD MODEL AT ZERO AND FINITE TEMPERATURE
RESULTS
SUMMARY AND DISCUSSION
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